Effect of Cr substitution on magnetic and magnetic entropy change of La0.65Eu0.05Sr0.3Mn1−xCrxO3 (0.05≤x≤0.15) rhombohedral nanocrystalline near room temperature
We have studied the effect of Cr substitution on magnetic and magnetocaloric properties in nanocrystalline La0.65Eu0.05Sr0.3Mn1−xCrxO3 (x=0.05, 0.1 and 0.15). The materials were prepared using the Pechini sol–gel method. All the studied samples were crystallized into a single phase rhombohedral stru...
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creator | Bellouz, R. Oumezzine, M. Hlil, E.K. Dhahri, E. |
description | We have studied the effect of Cr substitution on magnetic and magnetocaloric properties in nanocrystalline La0.65Eu0.05Sr0.3Mn1−xCrxO3 (x=0.05, 0.1 and 0.15). The materials were prepared using the Pechini sol–gel method. All the studied samples were crystallized into a single phase rhombohedral structure with R−3C space group. Magnetic measurements indicate that the ferromagnetic double exchange interaction is weakened with increasing Cr concentration, resulting in a shift in TC from 338K to 278K as x varied between 0.05 and 0.15. Detailed analyzes in the vicinity of the ferromagnetic (FM)–paramagnetic (PM) phase-transition temperature prove the samples undergoing a second-order phase transition. The magnetocaloric effect is calculated from the measurement of initial isothermal magnetization versus magnetic field at various temperatures. The maximum magnetic entropy change |ΔSMmax| is found to decrease with increasing of Cr content from 4.04J/KgK for x=0.05–0.78J/KgK for x=0.15 upon 5T applied field change.
The relative cooling power (RCP) of La0.65Eu0.05Sr0.3Mn1−xCrxO3 series is nearly 54% of pure Gd, which will be an interesting system for application in room temperature refrigeration.
•Nanocrystalline materials La0.65Eu0.05Sr0.3Mn1−xCrxO3 were obtained.•The Cr substitution decreases the TC from 338K for x=0.05–278K for x=0.15.•The relative cooling power of La0.65Eu0.05Sr0.3Mn1−xCrxO3 is nearly 54% of pure Gd.•Arrott plot analyses was applied to study the order of the magnetic transition.•La0.65Eu0.05Sr0.3Mn1−xCrxO3 samples show second order PM–FM transition at T=TC. |
doi_str_mv | 10.1016/j.jmmm.2014.09.053 |
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The relative cooling power (RCP) of La0.65Eu0.05Sr0.3Mn1−xCrxO3 series is nearly 54% of pure Gd, which will be an interesting system for application in room temperature refrigeration.
•Nanocrystalline materials La0.65Eu0.05Sr0.3Mn1−xCrxO3 were obtained.•The Cr substitution decreases the TC from 338K for x=0.05–278K for x=0.15.•The relative cooling power of La0.65Eu0.05Sr0.3Mn1−xCrxO3 is nearly 54% of pure Gd.•Arrott plot analyses was applied to study the order of the magnetic transition.•La0.65Eu0.05Sr0.3Mn1−xCrxO3 samples show second order PM–FM transition at T=TC.</description><identifier>ISSN: 0304-8853</identifier><identifier>EISSN: 1873-4766</identifier><identifier>DOI: 10.1016/j.jmmm.2014.09.053</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Magnetic property ; Magnetocaloric effect ; Nanocrystalline material ; Physics ; X-ray diffraction</subject><ispartof>Journal of magnetism and magnetic materials, 2015-02, Vol.375, p.136-142</ispartof><rights>2014 Elsevier B.V.</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c334t-abb5fc8c357f59e4e79f424d0c29cfc908b19e339e8e01f94da56490b384b713</citedby><cites>FETCH-LOGICAL-c334t-abb5fc8c357f59e4e79f424d0c29cfc908b19e339e8e01f94da56490b384b713</cites><orcidid>0000-0001-9262-3819 ; 0000-0002-6919-8778</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.jmmm.2014.09.053$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>230,314,778,782,883,3539,27911,27912,45982</link.rule.ids><backlink>$$Uhttps://hal.science/hal-01708390$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Bellouz, R.</creatorcontrib><creatorcontrib>Oumezzine, M.</creatorcontrib><creatorcontrib>Hlil, E.K.</creatorcontrib><creatorcontrib>Dhahri, E.</creatorcontrib><title>Effect of Cr substitution on magnetic and magnetic entropy change of La0.65Eu0.05Sr0.3Mn1−xCrxO3 (0.05≤x≤0.15) rhombohedral nanocrystalline near room temperature</title><title>Journal of magnetism and magnetic materials</title><description>We have studied the effect of Cr substitution on magnetic and magnetocaloric properties in nanocrystalline La0.65Eu0.05Sr0.3Mn1−xCrxO3 (x=0.05, 0.1 and 0.15). The materials were prepared using the Pechini sol–gel method. All the studied samples were crystallized into a single phase rhombohedral structure with R−3C space group. Magnetic measurements indicate that the ferromagnetic double exchange interaction is weakened with increasing Cr concentration, resulting in a shift in TC from 338K to 278K as x varied between 0.05 and 0.15. Detailed analyzes in the vicinity of the ferromagnetic (FM)–paramagnetic (PM) phase-transition temperature prove the samples undergoing a second-order phase transition. The magnetocaloric effect is calculated from the measurement of initial isothermal magnetization versus magnetic field at various temperatures. The maximum magnetic entropy change |ΔSMmax| is found to decrease with increasing of Cr content from 4.04J/KgK for x=0.05–0.78J/KgK for x=0.15 upon 5T applied field change.
The relative cooling power (RCP) of La0.65Eu0.05Sr0.3Mn1−xCrxO3 series is nearly 54% of pure Gd, which will be an interesting system for application in room temperature refrigeration.
•Nanocrystalline materials La0.65Eu0.05Sr0.3Mn1−xCrxO3 were obtained.•The Cr substitution decreases the TC from 338K for x=0.05–278K for x=0.15.•The relative cooling power of La0.65Eu0.05Sr0.3Mn1−xCrxO3 is nearly 54% of pure Gd.•Arrott plot analyses was applied to study the order of the magnetic transition.•La0.65Eu0.05Sr0.3Mn1−xCrxO3 samples show second order PM–FM transition at T=TC.</description><subject>Magnetic property</subject><subject>Magnetocaloric effect</subject><subject>Nanocrystalline material</subject><subject>Physics</subject><subject>X-ray diffraction</subject><issn>0304-8853</issn><issn>1873-4766</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp9kcFq3DAQhkVpoNukL9CTjs3B7mgl2xL0EpZNU9iSQ3MXsjzKarGlRdaG3Tdor3mGQt8rT1KbLe2tICFm-D9pxEfIewYlA1Z_3JW7YRjKJTBRgiqh4q_IgsmGF6Kp69dkARxEIWXF35C347gDmJKyXpBfa-fQZhodXSU6Htox-3zIPgY6rcE8BszeUhO6fwWGnOL-RO3WhEec0Y2Bsq7WB5he_pag5F8De_n-fFyl4z2nH-b2y4-fx2lP81bXNG3j0MYtdsn0NJgQbTqN2fS9D0gDmkRTjAPNOOwxmXxIeEUunOlHfPfnvCQPt-uH1V2xuf_8ZXWzKSznIhembStnpeVV4yqFAhvlxFJ0YJfKOqtAtkwh5wolAnNKdKaqhYKWS9E2jF-S6_O1W9PrffKDSScdjdd3Nxs994A1ILmCpzm7PGdtiuOY0P0FGOjZit7p2YqerWhQerIyQZ_OEE6fePKY9Gg9BoudT5MH3UX_P_w3sQaYtg</recordid><startdate>20150201</startdate><enddate>20150201</enddate><creator>Bellouz, R.</creator><creator>Oumezzine, M.</creator><creator>Hlil, E.K.</creator><creator>Dhahri, E.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0001-9262-3819</orcidid><orcidid>https://orcid.org/0000-0002-6919-8778</orcidid></search><sort><creationdate>20150201</creationdate><title>Effect of Cr substitution on magnetic and magnetic entropy change of La0.65Eu0.05Sr0.3Mn1−xCrxO3 (0.05≤x≤0.15) rhombohedral nanocrystalline near room temperature</title><author>Bellouz, R. ; Oumezzine, M. ; Hlil, E.K. ; Dhahri, E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c334t-abb5fc8c357f59e4e79f424d0c29cfc908b19e339e8e01f94da56490b384b713</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Magnetic property</topic><topic>Magnetocaloric effect</topic><topic>Nanocrystalline material</topic><topic>Physics</topic><topic>X-ray diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bellouz, R.</creatorcontrib><creatorcontrib>Oumezzine, M.</creatorcontrib><creatorcontrib>Hlil, E.K.</creatorcontrib><creatorcontrib>Dhahri, E.</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Journal of magnetism and magnetic materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bellouz, R.</au><au>Oumezzine, M.</au><au>Hlil, E.K.</au><au>Dhahri, E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of Cr substitution on magnetic and magnetic entropy change of La0.65Eu0.05Sr0.3Mn1−xCrxO3 (0.05≤x≤0.15) rhombohedral nanocrystalline near room temperature</atitle><jtitle>Journal of magnetism and magnetic materials</jtitle><date>2015-02-01</date><risdate>2015</risdate><volume>375</volume><spage>136</spage><epage>142</epage><pages>136-142</pages><issn>0304-8853</issn><eissn>1873-4766</eissn><abstract>We have studied the effect of Cr substitution on magnetic and magnetocaloric properties in nanocrystalline La0.65Eu0.05Sr0.3Mn1−xCrxO3 (x=0.05, 0.1 and 0.15). The materials were prepared using the Pechini sol–gel method. All the studied samples were crystallized into a single phase rhombohedral structure with R−3C space group. Magnetic measurements indicate that the ferromagnetic double exchange interaction is weakened with increasing Cr concentration, resulting in a shift in TC from 338K to 278K as x varied between 0.05 and 0.15. Detailed analyzes in the vicinity of the ferromagnetic (FM)–paramagnetic (PM) phase-transition temperature prove the samples undergoing a second-order phase transition. The magnetocaloric effect is calculated from the measurement of initial isothermal magnetization versus magnetic field at various temperatures. The maximum magnetic entropy change |ΔSMmax| is found to decrease with increasing of Cr content from 4.04J/KgK for x=0.05–0.78J/KgK for x=0.15 upon 5T applied field change.
The relative cooling power (RCP) of La0.65Eu0.05Sr0.3Mn1−xCrxO3 series is nearly 54% of pure Gd, which will be an interesting system for application in room temperature refrigeration.
•Nanocrystalline materials La0.65Eu0.05Sr0.3Mn1−xCrxO3 were obtained.•The Cr substitution decreases the TC from 338K for x=0.05–278K for x=0.15.•The relative cooling power of La0.65Eu0.05Sr0.3Mn1−xCrxO3 is nearly 54% of pure Gd.•Arrott plot analyses was applied to study the order of the magnetic transition.•La0.65Eu0.05Sr0.3Mn1−xCrxO3 samples show second order PM–FM transition at T=TC.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.jmmm.2014.09.053</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0001-9262-3819</orcidid><orcidid>https://orcid.org/0000-0002-6919-8778</orcidid></addata></record> |
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subjects | Magnetic property Magnetocaloric effect Nanocrystalline material Physics X-ray diffraction |
title | Effect of Cr substitution on magnetic and magnetic entropy change of La0.65Eu0.05Sr0.3Mn1−xCrxO3 (0.05≤x≤0.15) rhombohedral nanocrystalline near room temperature |
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